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Goos-H(a)nchen(GH)位移只有波长数量级,在实验测量上比较困难.提出了一种基于液晶光阀(LCLV)和光束分析仪(LBP)直接测量GH位移的新方法.研究了LCLV对光偏振态调制的特性,结果发现,当外接电压发生变化时,光的偏振态也随之变化.利用LCLV对光偏振态的调制和LBP记录光斑的重心位置的变化,直接测量出TE和TM两种偏振态入射时棱镜单界面反射光束的GH位移差.这个探测方法简单,不需要复杂的外部处理电路,且实验结果与理论结果很吻合,此方法也可以进一步直接测量二维位移.

参考文献

[1] Goos F,H(a)nchen H.Ein neuer and fundamentaler versuch zur totalreflexion[J].Ann.Phys.,1947,1:333.
[2] Artmann K.Berechnung der Seitenversetzung des total reflektieren Strahles[3].Ann.Phys.,1948,2:87.
[3] Renard R H.Total reflection:a new evaluation of the Goos-H(a)nchen shift[J].J.Opt.Soc.Am.,1964,54(10):1190.
[4] McGuirk M,Caruiglia C K.An angular spectrum representation approach to the Goos-H(a)nchen shift[J].J.Opt.Soc.Am.,1977,67(1):103.
[5] Costa de Beauregard O,Imbert C,Lévy Y.Observation of shifts in total reflection of a light beam by a multilayered structure[J].Phys.Rev.D,1977,15:3553.
[6] Gilles H,Girard S,Hamel J.Simple technique for measuring the Goos-H(a)nchen effect with polarization modulation and a position-sensitive detector[J].Opt.Lett.,2002,27(16):1421.
[7] Yin X B.Large positive and negative lateral optical beam displacements due to surface plasmon resonance[J].Appl.Phys.Lett.,2004,85(3):372.
[8] Chen L,Cao Z Q,Ou F C,et al.Observation of large positive and negative lateral shifts of a reflected beam from symmetrical metal-cladding waveguides[J].Opt.Lett.,2007,32(11):1432.
[9] Wang Y,Cao Z Q,Li H G,et al.Electric control of spatial beam position based on the Goos-H(a)nchen effect[J].Appl.Phys.Lett.,2008,93(3):091103.
[10] Cowan J J,Anicin B.Longitudinal and transverse displacements of a bounded microwave beam at total internal reflection[J].J.Opt.Soc.Am.B,1977,67:1307.
[11] Haibel A,Nimtz G,Stahofen A A.Frustrated total reflection:The double-prism revisited[J].Phys.Rev.E,2001,63(4):047601.
[12] Muller D,Tharanga D,Stahlhofen A A,et al.Nonspecular shifts of microwaves in partial reflection[J].EuroPhysics Letters,2006,73(4):526.
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